Haven't looked back on that thread in years... but the end result should be in mg... would need to go through the calc to check.
At the time I used the formula to confirm/verify a number of styli that had ETM specs...
The difficult bit wasn't this formula, which I found in published white papers... but deducting the LCR response from the measured response so you can reliably identify the ResF
Did you look at the graph I posted? Are you in doubt of the resonant frequency in that graph? Don't think LCR response would change that, other than amplitude. Also, look at the graph of the AT24 below.
The problem of measuring ultrasonics is, a) some carts roll off early and b) phonostage must be flat to 50kHz. Second, a sweep has very little energy, so a pink noise track is more likely to show the peaks. A sweep will also present a bunch of harmonics to whatever fundamental it's playing. A pink track works better, 20kHz will do. However, if you have music tracks with sufficient energy in the HF area, it can be visible by the right sampling method, e.g. FFT of a complete LP side. It just about exciting resonances.
Audio Technica AT-24 with custom VMN40ML stylus, made by Delta667. 30kHz pink.
Not much to see in fundamentals, but that 42kHz peak is hard to miss. (From 68KHz we see Motu M4 ultrasonic noisetake over).
This is a Sony XL-35 with SAS/B. No ultrasonic peaks to see, cart rolls off.
A different way of finding ResF could be treating the cantilever as a string. We know materials, in this case boron. We know dimensions - cylinder of 0,28mm x 7mm. Lengths vary, but not much. We know the physical properties of the materials, boron, in this case.
en.wikipedia.org
en.wikipedia.org
Anyone up for maths?